Coupled Map Lattices (CMLs) were introduced as suitable models to study the behaviour of spatially extended dynamical systems [1]}. These systems are defined on a discrete space-time, but with state variables that can take continuous values. Their behaviours range from ordered wave-like patterns to spatio-temporal chaos (i.e., turbulence) [2]}, [3]}, [4]}, [5]}. CMLs have also been generalised to include non-local interactions [6]}, either by using distance-dependent functions [7]}, [8]}, [9]} or by replacing the lattice regularity with complex graphs [10]}, [11]}, [12]}, [13]}, and delayed interactions [14]}, [15]}, [16]}. Overall, CMLs (and their generalisations) have allowed to deepen our understanding of complex behaviours, such as intermittence [17]}, [18]}, chimera states [19]}, [20]}, [21]}, and synchronisation [22]}, [23]}, [24]}, [25]}.
